In this section we explain how the Chazy equation arises from a 3-dimensional Frobenius manifold. We follow Dubrovin's notes [1]}, [2]}.
Let dim \(M = 3\) , and consider the potential function
\(F(t)= \frac{1}{2} \big (t^1\big )^2t^3 + \frac{1}{2} t^1\big (t^2\big )^2 - \frac{\big (t^2\big )^4}{16}\gamma \big (t^3\big ),\) 
